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import numpy as np | |
def neutrino_data(): | |
'''From arxiv:1405.7540 (table I) | |
and asumming a Normal Hierarchy: | |
Output: | |
mnu1in: laightest neutrino mass | |
Dms2: \Delta m^2_{12} | |
Dma2: \Delta m^2_{13} | |
ThetSol,ThetAtm,ThetRec: in radians | |
''' | |
Dms2=np.array([7.11e-5, 7.60e-5, 8.18e-5])*1e-18 # In GeV | |
Dma2=np.array([2.30e-3, 2.48e-3, 2.65e-3])*1e-18 # In GeV | |
#input real values: | |
# | |
ThetSol = np.array([0.278, 0.323, 0.375]) | |
ThetAtm = np.array([0.392, 0.567, 0.643]) | |
ThetRec = np.array([0.0177, 0.0234, 0.0294]) | |
mnu1in=1E-5*1E-9 | |
return mnu1in,Dms2,Dma2,ThetSol,ThetAtm,ThetRec | |
def CasasIbarra(ranMnu=True,bestfit=True): | |
#import numpy as np | |
if ranMnu==True: | |
bestfit=True | |
mnu1in,Dms2,Dma2,ThetSol,ThetAtm,ThetRec=neutrino_data() | |
# Phases of the PMNS matrix | |
phases1=np.random.uniform(0.,0.0*np.pi,3) # cero value for all phases | |
delta=1.*(0 if ranMnu else phases1[0]) | |
eta1 =1.*(0 if ranMnu else phases1[1]) | |
eta2 =1.*(0 if ranMnu else phases1[2]) | |
mnu1=1.*(mnu1in if bestfit else 10**((np.log10(2.5e-3)-np.log10(1e-9))*np.random.uniform(0,1)+np.log10(1e-9))*1e-9) | |
mnu2=1.*(np.sqrt(Dms2[1]+mnu1in**2) if bestfit else np.sqrt(np.random.uniform(Dms2[0],Dms2[2]) + mnu1**2) ) | |
mnu3=1.*(np.sqrt(Dma2[1]+mnu1in**2) if bestfit else np.sqrt(np.random.uniform(Dma2[0],Dma2[2]) + mnu1**2) ) | |
# Square root of left-handed neutrino mass matrix | |
DMnu = np.diag( [np.sqrt(mnu1),np.sqrt(mnu2),np.sqrt(mnu3)] ) | |
#print "NEUTRINOS",mnu1,mnu2,mnu3 | |
# Mixing angles (up 3 sigma range) | |
t12 = 1.*( np.arcsin(np.sqrt(ThetSol[1])) if bestfit else np.arcsin(np.sqrt(np.random.uniform(ThetSol[0],ThetSol[2])))) | |
t23 = 1.*( np.arcsin(np.sqrt(ThetAtm[1])) if bestfit else np.arcsin(np.sqrt(np.random.uniform(ThetAtm[0],ThetAtm[2])))) | |
t13 = 1.*( np.arcsin(np.sqrt(ThetRec[1])) if bestfit else np.arcsin(np.sqrt(np.random.uniform(ThetRec[0],ThetRec[2])))) | |
# Building PMNS matrix | |
U12 = np.array([ [np.cos(t12), np.sin(t12),0], [-np.sin(t12), np.cos(t12),0], [0,0,1.0] ]) | |
U13 = np.array([ [np.cos(t13),0, np.sin(t13)* np.exp(-delta*1j)], [0,1.0,0], [-np.sin(t13)*np.exp(delta*1j),0, np.cos(t13)] ]) | |
U23 = np.array([ [1.0,0,0], [0, np.cos(t23), np.sin(t23)], [0, -np.sin(t23), np.cos(t23)] ]) | |
Uphases = np.array([ [np.exp(eta1*1j),0,0], [0, np.exp(eta2*1j),0], [0,0,1.0] ]) | |
U = np.dot(U23,np.dot(U13,np.dot(U12,Uphases))) | |
return U | |
if __name__=='__main__': | |
print( CasasIbarra(ranMnu=True) ) |
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